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Reaction-diffusion-convection problems in unbounded cylinders.

Rozenn Texier-Picard, Vitaly A. Volpert (2003)

Revista Matemática Complutense

The work is devoted to reaction-diffusion-convection problems in unbounded cylinders. We study the Fredholm property and properness of the corresponding elliptic operators and define the topological degree. Together with analysis of the spectrum of the linearized operators it allows us to study bifurcations of solutions, to prove existence of convective waves, and to make some conclusions about their stability.

Regularity criterion for 3D Navier-Stokes equations in terms of the direction of the velocity

Alexis Vasseur (2009)

Applications of Mathematics

In this short note we give a link between the regularity of the solution u to the 3D Navier-Stokes equation and the behavior of the direction of the velocity u / | u | . It is shown that the control of Div ( u / | u | ) in a suitable L t p ( L x q ) norm is enough to ensure global regularity. The result is reminiscent of the criterion in terms of the direction of the vorticity, introduced first by Constantin and Fefferman. However, in this case the condition is not on the vorticity but on the velocity itself. The proof, based on very...

Remark on regularity of weak solutions to the Navier-Stokes equations

Zdeněk Skalák, Petr Kučera (2001)

Commentationes Mathematicae Universitatis Carolinae

Some results on regularity of weak solutions to the Navier-Stokes equations published recently in [3] follow easily from a classical theorem on compact operators. Further, weak solutions of the Navier-Stokes equations in the space L 2 ( 0 , T , W 1 , 3 ( 𝛺 ) 3 ) are regular.

Résultats d’existence dans des espaces critiques pour le système de la MHD inhomogène

Hammadi Abidi, Taoufik Hmidi (2007)

Annales mathématiques Blaise Pascal

Nous démontrons dans cet article que le système MHD tridimensionnel à densité et viscosité variables est localement bien posé lorsque ( ρ 0 - 1 - 1 , u 0 , B 0 ) B ˙ p 1 3 p ( 3 ) × B ˙ p 1 3 p - 1 ( 3 ) × B ˙ p 1 3 p - 1 ( 3 ) , pour p ] 1 , 3 ] et la densité initiale est proche d’une constante strictement positive. Nous démontrons également un résultat d’existence et d’unicité dans l’espace de Sobolev H 3 2 + α ( 3 ) × H 3 2 - 1 + α ( 3 ) × H 3 2 - 1 + α ( 3 ) pour α > 0 , sans aucune condition de petitesse sur la densité.

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